Tunable deconfined quantum criticality and interplay of different valence-bond solid phases
Zhao Bowen1, Takahashi Jun2, 1, Sandvik Anders W.1, 2, †
       

Distribution of the cVBS order parameter defined in Eq. (3b) for L = 32 systems with h = 0 at g = 0.80 in (a) and g = 0.78 in (b). In these calculations β=4L . The horizontal and vertical axes correspond to Re {mc} and Im {mc}, respectively. The color scale corresponds to a linear mapping from 0 to maximal probability density in each of the panels. The deviations from perfect Z4 symmetry in both (a) and (b) are due to slow migration of the VBS angle ϕ in the simulations.